Mass, Gas and Galaxies in the Abell 901/902 Supercluster
Mass, Gas and Galaxies in the Abell 901/902 Supercluster
Mass, Gas and Galaxies in the Abell 901/902 Supercluster
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<strong>Mass</strong>, <strong>Gas</strong> <strong>and</strong> <strong>Galaxies</strong> <strong>in</strong> <strong>the</strong> <strong>Abell</strong><br />
<strong>901</strong>/<strong>902</strong> <strong>Supercluster</strong><br />
Ca<strong>the</strong>r<strong>in</strong>e Heymans<br />
on behalf of <strong>the</strong> STAGES collaboration<br />
(PI: Meghan Gray)<br />
University of British Columbia, Vancouver.<br />
Canadian Institute for Theoretical Astrophysics, Toronto.<br />
Institute d’Astrophysique de Paris.
STAGES<br />
• 80 orbit mosaic<br />
• ACS + WFPC2/NIC3<br />
parallels<br />
• science exploitation<br />
underway<br />
• second largest HST<br />
mosaic<br />
• sister survey to GEMS/<br />
CDFS<br />
• Data public 20th Feb<br />
2008!<br />
Nott<strong>in</strong>gham<br />
M Gray (PI)<br />
K Lane<br />
A Aragón-Salamanca<br />
O Alma<strong>in</strong>i<br />
I Trujillo<br />
Ed<strong>in</strong>burgh<br />
D Bacon<br />
A Taylor<br />
Oxford<br />
C Wolf<br />
Innsbruck<br />
M Barden<br />
E van Kampen<br />
image: COMBO-17<br />
Collaborators<br />
Texas<br />
S Joghee<br />
J Caldwell<br />
F Barazza<br />
HIA<br />
Victoria<br />
C Peng<br />
UBC<br />
C Heymans<br />
L Van Waerbeke<br />
Arizona<br />
C Papovitch<br />
MPIA Heidelberg<br />
HW Rix<br />
E Bell<br />
K Meisenheimer<br />
R Somerville<br />
S Koposov<br />
K Jahnke<br />
B Häußler<br />
X Zheng<br />
A Pasquali<br />
U<strong>Mass</strong><br />
D McIntosh<br />
Columbia<br />
B Johnson<br />
AIP Postdam<br />
L Witozski<br />
A Boehm<br />
CAHA<br />
S Sanchez<br />
ESO/Chile<br />
R Gilmour<br />
Waterloo<br />
M Balogh
Ca<strong>the</strong>r<strong>in</strong>e Heymans LBL 22nd Jan 2008
Outl<strong>in</strong>e<br />
✴ The STAGES survey<br />
• Galaxy evolution <strong>in</strong> dense environments<br />
✴ “See<strong>in</strong>g <strong>the</strong> <strong>in</strong>visible”: mapp<strong>in</strong>g <strong>the</strong> dark<br />
matter environment of <strong>Abell</strong> <strong>901</strong>/<strong>902</strong><br />
• Weak gravitational lens<strong>in</strong>g<br />
✴ First galaxy evolution results from <strong>the</strong> <strong>Abell</strong><br />
<strong>901</strong>/<strong>902</strong> laboratory<br />
Ca<strong>the</strong>r<strong>in</strong>e Heymans LBL 22nd Jan 2008
The <strong>Abell</strong> <strong>901</strong>/<strong>902</strong> <strong>Supercluster</strong><br />
30x30 arcm<strong>in</strong> image of <strong>the</strong> A<strong>901</strong>/2 supercluster at z=0.165<br />
Ca<strong>the</strong>r<strong>in</strong>e Heymans LBL 22nd Jan 2008
A<strong>901</strong>a<br />
A<strong>901</strong>b<br />
A<strong>902</strong> SW group<br />
Ca<strong>the</strong>r<strong>in</strong>e Heymans Ground-based images from COMBO-17<br />
LBL 22nd Jan 2008
QE (%)<br />
λ / nm<br />
COMBO-17<br />
Wolf et al 2004<br />
σz ∼ 0.02(1 + z)<br />
✴ 5 broad b<strong>and</strong> + 12<br />
narrow b<strong>and</strong> filters<br />
✴ Photometric redshifts to<br />
R
STAGES: Space Telescope A<strong>901</strong>/<strong>902</strong> Galaxy Evolution Survey<br />
Hubble Space Telescope<br />
(M.E Gray)<br />
COMBO-17 survey<br />
(C. Wolf)<br />
Omega2000 @ Calar Alto<br />
(K. Meisenheimer)<br />
2dF spectrograph<br />
(M. E. Gray)<br />
XMM-Newton<br />
(R. Gilmour)<br />
Spitzer<br />
(E. F. Bell)<br />
GALEX<br />
(GALEX team)<br />
GMRT<br />
(D. Green)<br />
constra<strong>in</strong>ed simulations<br />
(E. van Kampen)<br />
80 orbit mosaic; ACS, NICMOS, WFPC<br />
morphologies, weak gravitational lens<strong>in</strong>g<br />
17-b<strong>and</strong> optical imag<strong>in</strong>g:<br />
photo-zs + SEDs for 15000 objects<br />
near-<strong>in</strong>frared extension (Y, J1, J2, H):<br />
M*, photo-zs<br />
spectroscopy of ~300 cluster galaxies:<br />
dynamics, star-formation histories<br />
90 ks X-ray imag<strong>in</strong>g/spectroscopy:<br />
ICM, AGN<br />
<strong>in</strong>frared imag<strong>in</strong>g (8 <strong>and</strong> 24 µm):<br />
obscured star formation, AGN<br />
NUV + FUV imag<strong>in</strong>g:<br />
unobscured star formation<br />
radio imag<strong>in</strong>g (610 <strong>and</strong> 1400MHz)<br />
obscured SF, AGN<br />
N-body + hydro + semi-analytic models<br />
dark matter, gas, galaxies<br />
Ca<strong>the</strong>r<strong>in</strong>e Heymans LBL 22nd Jan 2008
<strong>Mass</strong>ive ellipticals live<br />
<strong>in</strong> cluster cores<br />
What physical mechanism drives galaxy<br />
evolution <strong>in</strong> dense environments?<br />
Spirals, typically live <strong>in</strong> <strong>the</strong><br />
outskirts of <strong>the</strong> supercluster<br />
Ca<strong>the</strong>r<strong>in</strong>e Heymans LBL 22nd Jan 2008
LSB galaxy<br />
1: Galaxy-cluster gravitational <strong>in</strong>terations:<br />
Zoom <strong>in</strong>: Side on view Zoom <strong>in</strong>: Face on view<br />
Galaxy Harassment movie: The evolution of a low surface<br />
brightness galaxy as it falls <strong>in</strong>to a cluster (Moore et al 1998)<br />
Ca<strong>the</strong>r<strong>in</strong>e Heymans LBL 22nd Jan 2008
Ram pressure<br />
stripp<strong>in</strong>g: The<br />
turbulent history of a<br />
spiral galaxy as it falls<br />
through <strong>the</strong> hot ICM<br />
of a rich galaxy<br />
cluster (Quilis et al).<br />
2: Galaxy-cluster gas <strong>in</strong>terations:<br />
Ca<strong>the</strong>r<strong>in</strong>e Heymans LBL 22nd Jan 2008
3: Galaxy-cluster galaxy <strong>in</strong>terations:<br />
Galaxy Merger movie (Dub<strong>in</strong>ski et al)<br />
Ca<strong>the</strong>r<strong>in</strong>e Heymans LBL 22nd Jan 2008
1. Galaxy-cluster gas <strong>in</strong>teractions<br />
• ram-pressure stripp<strong>in</strong>g<br />
2. Galaxy-cluster gravitational <strong>in</strong>teractions<br />
• tidal truncation of galaxy dark matter halos<br />
3. Galaxy-galaxy <strong>in</strong>teractions<br />
What physical mechanism drives galaxy<br />
evolution <strong>in</strong> dense environments?<br />
• mergers (low-speed <strong>in</strong>teractions)<br />
• galaxy harrassment (high-speed<br />
<strong>in</strong>teractions)<br />
Any hope of disentangl<strong>in</strong>g<br />
<strong>the</strong>se effects requires<br />
knowledge of <strong>the</strong><br />
environment; <strong>in</strong> terms of<br />
mass, gas <strong>and</strong> galaxies.<br />
Ca<strong>the</strong>r<strong>in</strong>e Heymans LBL 22nd Jan 2008
Dark Matter is <strong>the</strong> underly<strong>in</strong>g structure of <strong>the</strong> Universe,<br />
dictat<strong>in</strong>g where <strong>and</strong> when galaxies form.<br />
Meghan Gray (University of Nott<strong>in</strong>gham) The Millennium <strong>and</strong> Ca<strong>the</strong>r<strong>in</strong>e Heymans simulation: (University Max of British Planck Columbia) Institute
See<strong>in</strong>g <strong>the</strong> <strong>in</strong>visible<br />
Meghan Gray (University of Nott<strong>in</strong>gham) <strong>and</strong> Ca<strong>the</strong>r<strong>in</strong>e Heymans (University of British Columbia)
See<strong>in</strong>g <strong>the</strong> <strong>in</strong>visible<br />
Meghan Gray (University of Nott<strong>in</strong>gham) <strong>and</strong> Ca<strong>the</strong>r<strong>in</strong>e Heymans (University of British Columbia)
lensed background<br />
galaxy z = 1.55<br />
lens galaxy z = 0.168<br />
Aragon-Salamanca et al <strong>in</strong> prep<br />
Meghan Gray (University of Nott<strong>in</strong>gham) <strong>and</strong> Ca<strong>the</strong>r<strong>in</strong>e Heymans (University of British Columbia)
The dark matter signature on <strong>the</strong> sky<br />
Matter<br />
Distant galaxies Dark Matter<br />
We can use <strong>the</strong> ‘lens<strong>in</strong>g’ signature of dark matter<br />
to tell us where is it <strong>and</strong> how much if it <strong>the</strong>re is.<br />
Ca<strong>the</strong>r<strong>in</strong>e Heymans LBL 22nd Jan 2008
Tangential arclets <strong>in</strong> A<strong>901</strong>a<br />
In <strong>the</strong> cores you can see <strong>the</strong> effect by eye.<br />
Ca<strong>the</strong>r<strong>in</strong>e Heymans LBL 22nd Jan 2008
How to make a dark matter map<br />
1. Obta<strong>in</strong> deep high resolution imag<strong>in</strong>g.<br />
2. Measure <strong>the</strong> ellipticities of distant<br />
galaxies.<br />
3. Account for all artifical sources of<br />
shear (eg <strong>in</strong>strumental distortions)<br />
that are typically more than an order<br />
of magnitude larger than <strong>the</strong> signal<br />
you’re try<strong>in</strong>g to detect (see STEP).<br />
4. Directly from GR you can relate <strong>the</strong><br />
measured shear to <strong>the</strong> projected mass.<br />
ACS PSF<br />
e i =e i source + γi<br />
= 0 γ ≈ <br />
Ca<strong>the</strong>r<strong>in</strong>e Heymans LBL 22nd Jan 2008
A<strong>901</strong>a<br />
In this analysis we use 60,000<br />
galaxies that are beh<strong>in</strong>d <strong>the</strong><br />
supercluster (65 gals per sq<br />
arcm<strong>in</strong>) to reconstruct <strong>the</strong> dark<br />
matter distribution<br />
A<strong>901</strong>b<br />
A<strong>902</strong> SW group<br />
Ca<strong>the</strong>r<strong>in</strong>e Heymans Ground-based images from COMBO-17<br />
LBL 22nd Jan 2008
130kpc resolution at supercluster redshift z=0.165<br />
Heymans et al 2008<br />
from 80 orbits of HST<br />
Ca<strong>the</strong>r<strong>in</strong>e Heymans LBL 22nd Jan 2008<br />
κ<br />
Contours show<br />
detections<br />
2σ, 4σ, 6σ
What about systematics?<br />
B<br />
E<br />
Lens<strong>in</strong>g only produces<br />
Emode distortions<br />
: systematics<br />
Ca<strong>the</strong>r<strong>in</strong>e Heymans LBL 22nd Jan 2008<br />
κ
M = 6.1 ± 0.8h −1 10 13 M⊙<br />
M/L = 131 ± 16hM⊙/L⊙<br />
M/M∗ = 32 ± 4<br />
ACS HST image<br />
A<strong>901</strong>a<br />
Infall<strong>in</strong>g X-ray<br />
group A<strong>901</strong>α<br />
Dark Matter density<br />
Ca<strong>the</strong>r<strong>in</strong>e Heymans LBL 22nd Jan 2008
A<strong>901</strong>b: <strong>the</strong> most<br />
massive <strong>and</strong> X-ray<br />
rich of <strong>the</strong> four<br />
clusters<br />
Dark Matter<br />
map resolves<br />
substructure<br />
M = 6.5 ± 1.3h −1 10 13 M⊙<br />
M/L = 165 ± 33hM⊙/L⊙<br />
M/M∗ = 42 ± 8<br />
ACS HST image Dark Matter density<br />
Ca<strong>the</strong>r<strong>in</strong>e Heymans LBL 22nd Jan 2008
A<strong>902</strong> has two peaks <strong>in</strong> <strong>the</strong><br />
dark matter distribution<br />
that are matched by two<br />
BCGs<br />
CBI z=0.46<br />
M = 3.3 ± 0.8h −1 10 13 M⊙<br />
M/L = 108 ± 25hM⊙/L⊙<br />
M/M∗ = 28 ± 6<br />
ACS HST image Dark Matter density<br />
Ca<strong>the</strong>r<strong>in</strong>e Heymans LBL 22nd Jan 2008
SW group<br />
M = 3.8 ± 0.5h −1 10 13 M⊙<br />
M/L = 176 ± 24hM⊙/L⊙<br />
M/M∗ = 41 ± 6<br />
ACS HST image Dark Matter density<br />
Ca<strong>the</strong>r<strong>in</strong>e Heymans LBL 22nd Jan 2008
<strong>Mass</strong> <strong>and</strong> Light<br />
M/L ∼ 100h −1 M⊙/L⊙<br />
Ca<strong>the</strong>r<strong>in</strong>e Heymans LBL 22nd Jan 2008
<strong>Mass</strong> to stellar mass ratio<br />
Ca<strong>the</strong>r<strong>in</strong>e Heymans LBL 22nd Jan 2008
Ground based Map from<br />
Gray et al 2002<br />
Why HST?<br />
Ca<strong>the</strong>r<strong>in</strong>e Heymans LBL 22nd Jan 2008<br />
κ<br />
Future space-based missions such as<br />
SNAP <strong>and</strong> DUNE are go<strong>in</strong>g to be vital<br />
for future dark matter observations<br />
κ
Why Hubble? ground-based<br />
Ca<strong>the</strong>r<strong>in</strong>e Heymans LBL 22nd Jan 2008
Why Hubble?<br />
STAGES<br />
answer: image quality <strong>and</strong> resolution allows us to detect <strong>the</strong> weak dark matter signature<br />
Ca<strong>the</strong>r<strong>in</strong>e Heymans LBL 22nd Jan 2008
Future telescopes <strong>in</strong> space: a<br />
quick note about depth<br />
✴ It’s not just about image quality.<br />
✴ For high resolution dark matter<br />
maps, you need depth<br />
γ ≈ <br />
✴ A smaller class telescope such as<br />
DUNE will need to observe much<br />
longer than SNAP to obta<strong>in</strong> deep<br />
enough data for simlarly high<br />
resolution observations<br />
DUNE ~ 1.2m<br />
SNAP ~2m<br />
Ca<strong>the</strong>r<strong>in</strong>e Heymans LBL 22nd Jan 2008
Ca<strong>the</strong>r<strong>in</strong>e Heymans LBL 22nd Jan 2008
STAGES:<br />
Space Telescope A<strong>901</strong>/<strong>902</strong> Galaxy Evolution Survey<br />
✴ The lens<strong>in</strong>g map is one key piece of a bigger puzzle<br />
✴ The larger picture looks at <strong>the</strong> l<strong>in</strong>k between galaxies<br />
<strong>and</strong> environment: nature vs nurture?<br />
✴ Look<strong>in</strong>g at <strong>the</strong> A<strong>901</strong>/<strong>902</strong> with multi-wavelength eyes<br />
we have assembled an ideal laboratory for study<strong>in</strong>g<br />
galaxy evolution<br />
✴ We are f<strong>in</strong>d<strong>in</strong>g that it is <strong>the</strong> outskirts of <strong>the</strong> cluster<br />
where galaxy transformations are occurr<strong>in</strong>g<br />
Ca<strong>the</strong>r<strong>in</strong>e Heymans LBL 22nd Jan 2008
galaxies<br />
dark<br />
matter<br />
STAGES: a laboratory for study<strong>in</strong>g galaxy<br />
evolution <strong>and</strong> environment<br />
“environment”<br />
hot<br />
gas<br />
• harrassment<br />
• strangulation<br />
• stripp<strong>in</strong>g<br />
• tidal truncation<br />
• merg<strong>in</strong>g<br />
• …<br />
star<br />
formation<br />
“galaxies”<br />
shapes<br />
active<br />
galactic<br />
nuclei<br />
sizes<br />
We need multiwavelength observations <strong>in</strong> order to get a full census of <strong>the</strong> supercluster.
Anatomy of a supercluster:<br />
a complex environment<br />
<strong>Mass</strong><br />
gravitational lens<strong>in</strong>g:<br />
Heymans et al 2008<br />
<strong>Gas</strong><br />
X-ray imag<strong>in</strong>g:<br />
Gilmour et al 2007<br />
Step 1: map out <strong>the</strong> environment<br />
<strong>Galaxies</strong><br />
optical imag<strong>in</strong>g<br />
Wolf et al 2004
<strong>Mass</strong>, <strong>Gas</strong> <strong>and</strong> <strong>Galaxies</strong><br />
Ca<strong>the</strong>r<strong>in</strong>e Heymans Ground-based images from COMBO-17<br />
LBL 22nd Jan 2008
hidden supermassive black hole<br />
Step 2: underst<strong>and</strong> <strong>the</strong> galaxies<br />
XMM GALEX HST Spitzer GMRT<br />
merg<strong>in</strong>g galaxy<br />
X-ray ultraviolet optical <strong>in</strong>frared<br />
radio<br />
dust obscuration
Galaxy Classification<br />
E B-V (dust)<br />
Wolf, Gray &<br />
Meisenheimer 2005<br />
Blue <strong>Galaxies</strong><br />
Old Red<br />
<strong>Galaxies</strong><br />
age [Myr]<br />
Dusty Red<br />
<strong>Galaxies</strong><br />
A population of dusty red star form<strong>in</strong>g galaxies<br />
make up 30% of <strong>the</strong> cluster red sequence<br />
A large population of anemic<br />
spirals/dusty red galaxies<br />
Lane et al 2007<br />
early-type late-type<br />
Ca<strong>the</strong>r<strong>in</strong>e Heymans LBL 22nd Jan 2008
Blue<br />
<strong>Galaxies</strong><br />
Step 3: connect galaxies <strong>and</strong> environment<br />
Dark<br />
matter<br />
contours<br />
Old Red<br />
<strong>Galaxies</strong><br />
Dusty Red<br />
<strong>Galaxies</strong><br />
Ca<strong>the</strong>r<strong>in</strong>e Heymans LBL 22nd Jan 2008
Step 3: connect galaxies <strong>and</strong> environment<br />
Result:<br />
it is <strong>the</strong> <strong>in</strong>termediate<br />
density or <strong>in</strong>fall regions<br />
where most of <strong>the</strong><br />
signatures of galaxy<br />
transformation are seen.<br />
Heiderman et al <strong>in</strong> prep<br />
Ca<strong>the</strong>r<strong>in</strong>e Heymans LBL 22nd Jan 2008
What causes galaxy evolution <strong>in</strong> dense<br />
✴ It’s not <strong>the</strong> gas<br />
environments?<br />
Prelim<strong>in</strong>ary conclusions:<br />
✴ It’s not high galaxy densities<br />
✴ The action seems to be where galaxies are first<br />
experienc<strong>in</strong>g <strong>the</strong> pull of dark matter<br />
✴ Our first f<strong>in</strong>d<strong>in</strong>gs are show<strong>in</strong>g a sweet-spot where<br />
galaxies become close enough, <strong>and</strong> are mov<strong>in</strong>g slow<br />
enough to <strong>in</strong>teract <strong>and</strong> transform.<br />
Ca<strong>the</strong>r<strong>in</strong>e Heymans LBL 22nd Jan 2008
Summary<br />
✴ STAGES is a multi-wavelength survey of <strong>the</strong> <strong>Abell</strong> <strong>901</strong>/<strong>902</strong><br />
supercluster.<br />
✴ The survey aims to dist<strong>in</strong>guish between <strong>the</strong> different physical<br />
mechanisms which drive galaxy evolution <strong>in</strong> dense environments.<br />
✴ Weak lens<strong>in</strong>g analysis of HST images permits high resolution<br />
dark matter “observations”.<br />
✴ Old Red <strong>Galaxies</strong> trace <strong>the</strong> underly<strong>in</strong>g dark matter distribution<br />
✴ Intermediate density regions key site for galaxy transformations<br />
✴ Current work br<strong>in</strong>g<strong>in</strong>g toge<strong>the</strong>r all different multi-wavelength<br />
cluster <strong>in</strong>formation to form a coherent underst<strong>and</strong><strong>in</strong>g of <strong>the</strong><br />
violent history of this supercluster<br />
Ca<strong>the</strong>r<strong>in</strong>e Heymans LBL 22nd Jan 2008